To solve this problem, we use the photoelectric effect's principle. According to Einstein's photoelectric equation: KEmax = hf - ϕ, where KEmax is the maximum kinetic energy of the emitted electrons, h is Planck's constant, f is the frequency of the incident light, and ϕ is the work function of the metal. Given conditions: 1. Frequency of the incident light = 2 × threshold frequency, resulting in speed v1. 2. Frequency increased to 5 × threshold frequency, resulting in speed v2. Assuming f0 is the threshold frequency and m is the electron's mass, derive two scenarios: For v1: h(2f0) = (1/2)mv12 + ϕ — (1). For v2: h(5f0) = (1/2)mv22 + ϕ — (2). Subtract equation (1) from (2): h(5f0) - h(2f0) = (1/2)mv22 - (1/2)mv12. Simplify: h(3f0) = (1/2)m(v22-v12) — (3). From (1): hf0 = ϕ. Substituting, equation (3) becomes: (3ϕ) = (1/2)m(v22-v12). Solve for v2: (2*3ϕ)/m = v22-v12, hence v22 = v12 + (6ϕ/m). From equation (1): hf0 = ϕ = (1/2)mv12. Thus, v22 = v12 + 3v12. Therefore, v2 = 2v1, leading to x = 2. The value of x is confirmed to be within the given range [2, 2].